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Hinton - The Fourth Dimension.pdf

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80<br />

THE FOURTH DIMENSION<br />

Let us consider a sphere of our three-dimensional<br />

z<br />

F<br />

D<br />

Fig. 44.<br />

Axis of x running towards<br />

the observer.<br />

matter having a definite<br />

thickness. To represent<br />

this thickness let us suppose<br />

that from every point<br />

of the sphere in fig. 44 rods<br />

project both ways, in and<br />

out, like D and F. We can<br />

only see the external portion,<br />

because the internal<br />

parts are hidden by the<br />

sphere.<br />

In this sphere the axis<br />

of x is supposed to come<br />

towards the observer, the<br />

axis of z to run up, the axis of y to go to the right.<br />

Now take the section determined by the xy plane.<br />

z<br />

w<br />

E<br />

Fig. 45.<br />

F<br />

C<br />

D<br />

y<br />

This will be a circle as<br />

shown in fig. 45. If we<br />

let drop the x axis, this<br />

circle is all we have of<br />

the sphere. Letting the<br />

w axis now run in the<br />

plane of the old x axis<br />

we have the space yzw<br />

and in this space all that<br />

we have of the sphere is<br />

the circle. Fig 45 then<br />

represents all that there<br />

is of the sphere in the<br />

space of yzw. In this space it is evident that the rods<br />

CD and EF can turn round the circumference as an axis.<br />

If the matter of the spherical shell is sufficiently extensible<br />

to allow the particles C and E to become as widely<br />

separated as they would in the positions D and F, then<br />

y

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